Circular dichroism of the “random” polypeptide chain

The circular dichroism (CD) spectrum of an unordered polypeptide chain does not correspond, as has been assumed heretofore, to that of a charged chain such as poly-L -glutamic acid or poly-L -lysine. The latter have been shown to have locally ordered structures with characteristic CD spectra. We have now obtained CD spectra of the unordered forms of the above synthetic, polypeptides, as well as of two fibrous proteins (collagen and feather keratin) and a globular protein (myoglobin). These spectra are all similar to that of unordered polyproline, having a negative band in the vicinity of 2000 mμ and no additional bands at longer wavelengths. The lack of structural uniqueness of the unordered polypeptide chain is emphasized by these studies.     

The calculated circular dichroism of polyproline II in the polarizability approximation

The circular dichroism (CD) spectrum of polyproline II (PPII) has heretofore been moderately well calculated from exciton theory only at the expense of assuming unreasonable chain conformations and accepting a conservative spectrum in the 180–250-nm region (which is not observed). We have incorporated far uv transitions in the polarizability approximation and, together with the π₂π* transition, have calculated the resulting correction to the exciton model. This has been accompanied by a modified assignment of the ππ* transition in PPII, and a simultaneous calculation of the absorption and CD spectra of the α-helix, β structure, PPI, and PPII. We obtain good agreement with the observed CD spectrum of PPII in the 180–250-nm region for acceptable chain conformations. In addition, we predict a negative CD into the far uv, in agreement with recent experimental observations. Our calculations also reproduce features of the far uv CD spectrum of the α-helix, and are in agreement with the CD spectra of the β chain and PPI. The calculated CD of the unordered polypeptide chain is not significantly influenced by far uv contributions, indicating that our previous calculation is valid for such a system. These results demonstrate the importance of incorporating far uv transitions in order to achieve an adequate theoretical explanation of the CD spectra of polypeptides.     

Effect of temperature on the circular dichroism spectra of polypeptides in the extended state

The circular dichroism (CD) spectra of poly-L -proline and of poly-L -glutamic acid and poly-L -lysine in their charged states have been studied as a function of temperature. The variation of CD spectra with temperature is inconsistent with the assignment of the spectrum of such charged polypetides to an unordered chain conformation, but does support our earlier assignment to a locally ordered structure—what we have called the extended helix conformation. These results also strengthen our previous assignment of the CD spectrum of an unordered chain, and indicate that three conformational states (α-helix, extended helix, and unordered) should be incorporated in our thinking about conformational transitions in polypeptides.     

Studies on bovine spleen cathepsin D

The purification procedure of cathepsin D which includes autolysis results in the destruction of the molecule to smaller polypeptide chains. Pure catepsin D obtained by the method which includes affinity chromatography, contains single polypeptide chain of 42000 daltons. The N-terminal amino acid is glycine. The specificity was studied using synthetic substrates. CD measurement of cathepsin D shows mainly unordered structure, about 26% of beta-structure and only 5% of alpha-helix. Binding of pepstatin shows pronounced changes in the CD spectrum between 250 and 300 nm; above 7.5 no interaction was observed.     

Conformational transition of hyaluronic acid in aqueous-organic solvent monitored by vacuum ultraviolet circular dichroism

The chiroptical transition of hyaluronic acid (HA) in aqueous-organic solvent has been investigated by circular dichroism (CD) spectroscopy into the vacuum ultraviolet region. The CD of HA changes dramatically, monitoring a cooperative transition as the dielectric constant of an aqueous solution is reduced by adding organic solvents. This transition results in a high-intensity CD band at 188 nm, indicating an ordered structure in the mixed solvent. Heating HA in the mixed solvent also causes a cooperative transition, reducing the CD to that found for the polymer in aqueous solution. In contrast, heating HA in aqueous solution results in small, noncooperative changes in the CD spectrum. This indicates an unordered structure in aqueous solution. The CD as the dielectric constant is reduced exhibits isodichroic points, showing that there are only two environments for chromophores contributing to the CD. This is confirmed by singular value decomposition of CD spectra recorded as a function of solvent composition, which shows the spectra to contain only two principal components. The data describing the thermally induced transition of HA in mixed solvent are not consistent with infinite cooperativity. The van't Hoff relation yields thermodynamic parameters for the conformational transition in terms of the cooperative unit of -60 kcal mol-1 for delta H degrees and -180 eu mol-1 for delta S degrees.     

Circular dichroism spectroscopy of fluorescent proteins

Circular dichroism (CD) spectra have been obtained from several variants of green fluorescent protein: blue fluorescent protein (BFP), enhanced cyan fluorescent protein (CFP), enhanced green fluorescent protein (GFP), enhanced yellow fluorescent protein (YFP), all from Aequorea victoria, and the red fluorescent protein from the coral species Discosoma (DsRed). We demonstrate that CD spectra in the spectral fingerprint region of the chromophore yield spectra that after normalization are not coincident with the normalized absorbance spectra of GFP, YFP and DsRed. On the other hand, the CD spectra of BFP and CFP coincide with the absorbance spectra. The resolution of absorption and CD spectra into Gaussian bands confirmed the location of the different electronic band positions of GFP and YFP as reported in the literature using other techniques. In the case of BFP and CFP the location of Gaussian bands provided information of the vibrational progression of the electronic absorption bands. The CD spectrum of DsRed is anomalous in the sense that the major CD band has a clear excitonic character. Far-UV CD spectra of GFP confirmed the presence of the high beta-sheet content of the polypeptide chain in the three-dimensional structure.     

Optical activity of simple cyclic amides in solution

The cyclic dipeptide, L -alanylglycyl anhydride, has been studied by optical rotatory dispersion; both L -alanylglycyl anhydride and the lactam, L -3-aminopyrrolidin-2-one, have been studied by circular dichroism. In hydroxylic solvents the circular dichroism spectra of 3-aminopyrrolidin-2-one can be attributed to an n–π* transition near 220 mμ and a π–π* transition near 190 mμ. In these solvents the optical activity of L -alanylglycyl anhydride can be explained as being due to contributions of n–π* transitions and a split π–π* transition. In acetonitrile, however, the circular dichroism spectrum of 3-aminopyrrolidin-2-one shows an additional apparent minimum near 200 mμ. The CD spectrum of the dipeptide is also quite distinctive in this solvent. The possible nature of the band at 200 mμ and the implications of these findings are discussed.     

Intrinsically unstructured proteins by design—electrostatic interactions can control binding,folding, and function of a helix‐loop‐helix heterodimer

Intrinsically disordered proteins that exist as unordered monomeric structures in aqueous solution at pH 7 but fold into four‐helix bundles upon binding to recognized polypeptide targets have been designed. NMR and CD spectra of the monomeric polypeptides show the hallmarks of unordered structures, whereas in the bound state they are highly helical. Analytical ultracentrifugation data shows that the polypeptides bind to their targets to form exclusively heterodimers at neutral pH. To demonstrate the relationship between binding, folding, and function, a catalytic site for ester hydrolysis was introduced into an unordered and largely inactive monomer, but that was structured and catalytically active in the presence of a specific polypeptide target. Electrostatic interactions between surface‐exposed residues inhibited the binding and folding of the monomers at pH 7. Charge–charge repulsion between ionizable amino acids was thus found to be sufficient to disrupt binding between polypeptide chains despite their inherent propensities for structure formation and may be involved in the folding and function of inherently disordered proteins in biology. Copyright © 2013 European Peptide Society and John Wiley & Sons, Ltd.     

Ca2+-induced conformational transitions of phosphorylated peptides

CD spectroscopic studies on protected peptides containing lysine and serine, or phosphoserine, and on serine-containing fragments of the neurofilament protein midsized subunit, both in the unphosphorylated and phosphorylated form, are reported. The introduction of the phosphoryl group was not found to have a significant spectral effect in aqueous solution. In trifluoroethanol (TFE), spectral shifts toward unordered (type U) spectra or the appearance of distorted spectra likely reflect the adoption of aperiodic polypeptide conformations due to salt bridge(s) between negatively charged phosphoserine and positive lysine side-chain groups. A turn-stabilizing effect of phosphorylation was also observed. CD-monitored titration experiments in TFE revealed a high conformational sensitivity of phosphopeptides toward Ca²⁺ ions. The appearance of the unordered spectra or spectral shifts were the sign of a bulk disordering effect of Ca²⁺ ions. Spectra with specific spectroscopic features reflect the formation of Ca²⁺complexes and the adoption of ordered unique backbone conformations. When ordered structures were obtained on addition of Ca²⁺ ions, the observed CD curves showed a resemblance to the spectrum of β-pleated sheets. This may originate from chain extension and the formation of β-pleated sheet segments fixed by Ca²⁺ bridges between PO₃H groups of adjacent peptide chains. The data clearly show that the effect of the Ca²⁺ ions is highly specific: the sequence, chain length, presence and distribution of charged side-chain groups, degree and site of phosphorylation, and environmental factors appear to be determining in the process of chain extension or β-sheet formation. © 1993 John Wiley & Sons, Inc.     

Conformation and aggregation of melittin: effect of pH and concentration of sodium dodecyl sulfate

The conformation of melittin, a surface-active polypeptide, in solution was studied by CD spectra between 190 and 240 nm. The molecule was essentially unordered (possibly with a trace of helix) in water without salt at neutral pH. Upon deprotonation of four of the six cationic groups at pH 12 the polypeptide became partially helical (about 35%). The addition of NaDodSO₄ to an aqueous melittin solution first caused the solution to become turbid but it became clear again in excess surfactant solution. The conformational changes depended on the molar NaDodSO₄/melittin ratio, R. With R from 2.34 to 23.4, the melittin solution was turbid and the polypeptide conformation was probably a mixture of α-helix and β-sheets. This was supported by the ir spectrum of the turbid solution, which indicated the presence of both conformations. With R = 46.8 or 468 (1 or 10 mM NaDodSO₄) the polypeptide conformation was characteristic of an α-helix, about 70–80% of the molecule, regardless of whether the surfactant was above or below its critical micelle concentration. This compared well with the x-ray results of 92% helix in crystals. The lower helicity of melittin in NaDodSO₄ solution might be attributed to the end effects that destabilize the first and last turn of an helix at its N- and C-terminus, respectively.     

Purification and characterization of potato lectin

Potato lectin (Solanum tuberosum agglutinin, STA), purified by affinity chromatography on tri-N-acetylchitotriose-Sepharose 6B, has Mr approximately 100,000, as estimated by gel filtration on Sephadex G-150 and is an aggregating system with a monomer Mr = 54,000, as estimated by sedimentation equilibrium analysis. Equilibrium dialysis showed that STA (dimer) has two binding sites for a specific sugar per molecule. STA has a high content of sugar, most of which is L-arabinose, and is rich in Hyp and Cys. On interaction with specific sugars, STA induced a UV difference spectrum having positive peaks at 292 and 285 nm characteristic of tryptophyl residues. The association constants with chitin oligosaccharides, determined from the intensities of the difference spectra at various concentrations of sugars, increased with increasing chain length of the sugar. Association constants obtained by frontal affinity chromatography of chitin oligosaccharides with STA-Sepharose were in good agreement with those obtained by difference spectra, whereas the association constants obtained by frontal affinity chromatography of STA with di- and tri-N-acetylchitotriose-Sepharose were much higher, presumably owing to the effect of multivalency of ligands. The CD spectra of STA in the far UV region indicate the presence of 40% of beta- and 60% of unordered form, and no alpha-helix conformation, which supports the structure suggested by the amino acid composition and the high content of sugar.     

Analysis of the circular dichroism spectrum of proteins using the convex constraint algorithm: a practical guide.

Due to the time scale of circular dichroism (CD) measurements, it is theoretically possible to deconvolute such a spectrum if the pure CD spectra differ significantly from one another. In the last decade several methods have been published aiming at obtaining the conformational weights, or percentages (which are the coefficients for a linear combination) of the so-called typical secondary structural elements making up the three-dimensional structure of proteins. Two methods that can be used to determine the secondary structures of proteins are described here. The first method, called LINCOMB, is a simple algorithm based on a least-squares fit with a set of reference spectra representing the known secondary structures and yielding an estimation of weights attributed to alpha-helix, beta-pleated sheet (mainly antiparallel), beta-turns, unordered form, and aromatic/disulfide (or nonpeptide) contributions of the protein being analyzed. This method requires a "template" or reference curve set, which was obtained from the second method. The second method, "convex constraint analysis," is a general deconvolution method for a CD spectra set of any variety of conformational type. The algorithm, based on a set of three constraints, is able to deconvolute a set of CD curves to its common "pure"-component curves and conformational weights. To analyze a single CD spectrum with this method, the spectrum is appended to the data set used as a reference data set. As a way to determine the reliability of the algorithm and provide a guideline to its usage, some applications are presented.     

Solvent effects on the conformation and far UV CD spectra of gramicidin

Solvent effects on the far-uv CD spectra of the polypeptide gramicidin have been studied systematically in a series of alcohols of increasing chain length, ranging from methanol to dodecanol. The effects observed are of two types: primary, involving a change in the equilibrium mixture of conformers present, and secondary, involving a shift in the spectral peak positions as a function of solvent polarizability. To quantitate the primary effect, the ratio of the individual conformers present was estimated by deconvolution of the spectra into their component species. For short chain length alcohols, both parallel and antiparallel double helices are found in considerable abundance. As the solvent chain length is increased and its polarity is decreased, the left-handed antiparallel double helical species is favored. For all alcohols with chain lengths of four or more carbon atoms, the ratio of the conformers present remains relatively constant. To quantitatively examine the secondary effect, the magnitudes of the spectral shifts on the dominant conformer (species 3) have been correlated with the dielectric constants and refractive indices of the solvents, thereby indicating what underlying physical properties are responsible for these shifts. This work thus demonstrates that for gramicidin, a flexible polypeptide, the solvent effects on the CD spectra can be resolved into two types: changes due to the mixture of conformers present and shifts in the spectral characteristics. Both effects need to be considered when interpreting CD spectra in terms of secondary structure for this and other polypeptides in nonaqueous solutions.     

Circular dichroism of the parallel β helical proteins pectate lyase C and E

The pectate lyases, PelC and PelE, have an unusual folding motif, known as a parallel β-helix, in which the polypeptide chain is coiled into a larger helix composed of three parallel β-sheets connected by loops having variable lengths and conformations. Since the regular secondary structure consists almost entirely of parallel β-sheets these proteins provide a unique opportunity to study the effect of parallel β-helical structure on circular dichroism (CD). We report here the CD spectra of PelC and PelE in the presence and absence of Ca²⁺, derive the parallel β-helical components of the spectra, and compare these results with previous CD studies of parallel β-sheet structure. The shape and intensity of the parallel β-sheet spectrum is distinctive and may be useful in identifying other proteins that contain the parallel β-helical folding motif. © 1995 Wiley-Liss, Inc.     

Structural composition of betaI- and betaII-proteins

Circular dichroism spectra of proteins are sensitive to protein secondary structure. The CD spectra of alpha-rich proteins are similar to those of model alpha-helices, but beta-rich proteins exhibit CD spectra that are reminiscent of CD spectra of either model beta-sheets or unordered polypeptides. The existence of these two types of CD spectra for beta-rich proteins form the basis for their classification as betaI- and betaII-proteins. Although the conformation of beta-sheets is largely responsible for the CD spectra of betaI-proteins, the source of betaII-protein CD, which resembles that of unordered polypeptides, is not completely understood. The CD spectra of unordered polypeptides are similar to that of the poly(Pro)II helix, and the poly(Pro)II-type (P2) structure forms a significant fraction of the unordered conformation in globular proteins. We have compared the beta-sheet and P2 structure contents in beta-rich proteins to understand the origin of betaII-protein CD. We find that betaII-proteins have a ratio of P2 to beta-sheet content greater than 0.4, whereas for betaI-proteins this ratio is less than 0.4. The beta-sheet content in betaI-proteins is generally higher than that in betaII-proteins. The origin of two classes of CD spectra for beta-rich proteins appears to lie in their relative beta-sheet and P2 structure contents.     

Water interaction differences determine the relative energetic stability of the polyproline II conformation of the alanine dipeptide in aqueous environments

Although subsequent studies have provided extensive support for the 1968 Tiffany and Krimm proposal (Biopolymers 6, 1379) that the polyproline II (PPII) conformation is a significant component of the structure of unordered polypeptide chains, two issues are still not fully resolved: the PPII persistence length in a chain and the source of its relative stability with respect to the β-conformation. We examine the latter question by studying the B97-D/6-31++G(**) energy, in the absence and presence of a reaction field, of the alanine dipeptide hydrated by various amounts of explicit waters and resolving this into its three components: the energies of the individual solvated peptides and water structures plus the interaction energy involving them. We find that the relative stability of the PPII conformation is determined mainly by the difference in the interaction energies of the water structures in the near-peptide layers.     

A simple model for the optical properties of chiral amides

The intramolecular charge-transfer model for the electronic structure of amides has been extended to include the effects of torsion about the peptide bond (Δω = ω – 180) and pyramidalization at the peptide nitrogen (θ_N). The model is used to calculate the absorption and CD spectra of nonplanar amides as a function of the angles Δω and θ_N. For cis-amides, the rotational strengths of the nπ* and ππ* transitions are much more sensitive to θ_N for a given value of Δω than is the case for trans-amides. The results from the model are compared with available experimental and previous theoretical treatments of such systems. The contributions of nonplanarity in amides to the CD of various polypeptide conformations is discussed. The effects should be negligible for α-helixes but may be quite significant in β-sheets and β-turns. The CD spectrum of unordered peptides would be readily explained if there were a significant bias toward negative Δω values in polypeptides of L-amino acids. However, the evidence currently available does not indicate such a bias.     

Distinct circular dichroism spectroscopic signatures of polyproline II and unordered secondary structures: Applications in secondary structure analyses

Circular dichroism (CD) spectroscopy is a valuable method for defining canonical secondary structure contents of proteins based on empirically‐defined spectroscopic signatures derived from proteins with known three‐dimensional structures. Many proteins identified as being “Intrinsically Disordered Proteins” have a significant amount of their structure that is neither sheet, helix, nor turn; this type of structure is often classified by CD as “other”, “random coil”, “unordered”, or “disordered”. However the “other” category can also include polyproline II (PPII)‐type structures, whose spectral properties have not been well‐distinguished from those of unordered structures. In this study, synchrotron radiation circular dichroism spectroscopy was used to investigate the spectral properties of collagen and polyproline, which both contain PPII‐type structures. Their native spectra were compared as representatives of PPII structures. In addition, their spectra before and after treatment with various conditions to produce unfolded or denatured structures were also compared, with the aim of defining the differences between CD spectra of PPII and disordered structures. We conclude that the spectral features of collagen are more appropriate than those of polyproline for use as the representative spectrum for PPII structures present in typical amino acid‐containing proteins, and that the single most characteristic spectroscopic feature distinguishing a PPII structure from a disordered structure is the presence of a positive peak around 220nm in the former but not in the latter. These spectra are now available for inclusion in new reference data sets used for CD analyses of the secondary structures of soluble proteins.     

Vibrational spectrum of the unordered polypeptide chain: A Raman study of feather keratin

Raman spectra of native and solubilized feather keratin have been obtained, and the amide I and amide III regions have been analyzed by band resolution techniques. The amide I region of the native form indicates that at least 64% of the protein has an antiparallel chain pleated sheet structure, the remainder being unordered. For the solubilized keratin all of the protein is in an unordered state. The amide III region is not as easily analyzed into component contributions. Normal vibration analyses on N-acetyl-L -alanine-N-methylamide support the conclusion that the amide III region is not as satisfactory as the amide I region in characterizing unordered structures. Even in the latter case caution must be used, since the observed amide I band is an average over the conformational distribution in the particular unordered system.     

Local structures in unfolded lysozyme and correlation with secondary structures in the native conformation: helix-forming or -breaking propensity of peptide segments

CD spectra of reduced and S-3-(trimethylated amino) propylated lysozyme (TMAP lysozyme) have been measured in various solutions containing guanidine hydrochloride or trifluoroethanol (TFE). The CD spectra indicate that there remain residual secondary structures in protein in aqueous solution. The addition of TFE further promotes the formation of secondary structures. In order to examine whether secondary structures are evenly induced over all the polypeptide chain, or locally at particular segments, the limited proteolysis of TMAP lysozyme by trypsin has been performed, and the CD spectra of all the final and intermediate products have been observed in solutions containing TFE. As a result, the fragments vary in a helix-forming propensity. The CD spectra of peptide fragments T5, T7, T9T10, T12T13, T14T15T16, and T17T18 are not significantly affected by the addition of TFE, where T refers to the nomenclature of R.E. Canfield [(1963), Journal of Biological Chemistry, Vol. 238, pp. 2691-2697]. They are fragments of a helix-breaking propensity. On the other hand, fragment I2 composed of T1-T4, and fragments T6T7, T8, and T11, attain secondary structures with the addition of TFE. They are fragments of a helix-forming propensity. Further, it is found that the fragments of a helix-forming propensity just correspond to the helical segments in native lysozyme. We examine the interactions between neighboring fragments, which contribute to the stabilization of local structures along the polypeptide chain.